Bohm Questions: What are Test Particles Good For?

  • Thread starter Hurkyl
  • Start date
In summary, particles in the Bohm interpretation of quantum mechanics are defined as having well-defined positions and momentums, but they do not have any actual effect on anything. They are more like hypothetical test particles used in analyzing force fields or space-time geometry. This raises questions about the usefulness of these particles in describing reality and how they can be reconciled with the fact that physical particles do interact with other things. The particles are necessary for solving the measurement problem and determining the mass and charge of particles. However, there are potential complications in quantizing the gauge independent degrees of freedom in non-Abelian Yang-Mills theories. Further development is needed in this area.
  • #36
Maaneli said:
You are welcome. Yes, I prefer the term "de Broglie-Bohm theory" because it gives due credit to Louis de Broglie's contributions. I think DGZ, who invented the term "Bohmian mechanics", should have instead invented terms like "Bellian mechanics" or "de Broglie-Bell theory/mechanics" or "de Broglie-Bohm-Bell theory", because Bell and de Broglie were the ones who advocated the first order guidance view, and deemphasized the quantum potential causal view, as DGZ have done. Bohm was never an advocate of the guidance view or the interpretations of DGZ, and personally was insulted (or so I was told) by the way his name was associated with the DGZ approach.

So if I have it right:

de Broglie-Bohm theory: the quantum potential is key; this is the version you support and is consistent with Bohm's views. Is ttn a follower of this as well? I assume that Passon is too?

DGZ version ("Bohmian mechanics"): the guidance condition is fundamental and the quantum potential is de-emphasized. Bell preferred this version, as I understand it. Is Demystifier in this camp (not asking you to speak for him, just wonder if you happen to know)?
 
Physics news on Phys.org
  • #37
Given the title of this thread, I have a question:

How does the dBB explain entangled photons a la PDC? OK, I see that the non-local character of the theory means that there is in principle a way to connect happenings at Alice with happenings at Bob, regardless of distance. But I would guess that for the Bell test answers to be properly correlated, that the quantum potential would need to be the same for both photons as long as they are entangled. Am I close? :)
 
  • #38
DrChinese said:
So if I have it right:

de Broglie-Bohm theory: the quantum potential is key; this is the version you support and is consistent with Bohm's views. Is ttn a follower of this as well? I assume that Passon is too?


Correction: In de Broglie-Bohm theory the quantum potential is not necessarily key - in other words, it does not represent Bohm's particular view of the equations of the theory. The term deBB theory is intended just to agnostically refer to all the properties of the theory (wavefunction, particles, quantum potential), and to the original contributions of both de Broglie and Bohm. In fact, de Broglie, who actually emphasized the guidance view, was the first to also coin the term "pilot wave theory". Bell was actually the first to use the term "de Broglie-Bohm" to refer to the theory originally discovered by both de Broglie and Bohm. Bohm used the term "causal interpretation" or the "ontological interpretation" to refer to his particular interpretation of the theory. Nowadays, researchers who want to stay out of this terminological disagreement typically just use the term "de Broglie-Bohm theory" or "pilot wave theory".

Travis is a staunch subscriber to the DGZ view and always uses the term Bohmian mechanics, as you may have noticed. I don't know though how aware he is of this terminological disagreement. Passon doesn't state his preference, as he uses all the terms in his papers.


DrChinese said:
DGZ version ("Bohmian mechanics"): the guidance condition is fundamental and the quantum potential is de-emphasized. Bell preferred this version, as I understand it. Is Demystifier in this camp (not asking you to speak for him, just wonder if you happen to know)?


Right. I don't know if Demystifier is in the DGZ camp, but in all his papers I have seen him use the term Bohmian mechanics almost exclusively. I suppose we could just ask him.


Demystifier, what do you think of this terminological disagreement?
 
  • #39
Maaneli said:
Travis is a staunch subscriber to the DGZ view and always uses the term Bohmian mechanics, as you may have noticed. I don't know though how aware he is of this terminological disagreement. Passon doesn't state his preference, as he uses all the terms in his papers.

Right. I don't know if Demystifier is in the DGZ camp, but in all his papers I have seen him use the term Bohmian mechanics almost exclusively. I suppose we could just ask him.

Demystifier, what do you think of this terminological disagreement?

The issue for me is that I am still learning about dBB/BM. Travis had never objected to me about the terminology, so what you say makes sense. He also talks about Bell's later writings a lot, so that makes sense too.

As I look into the issues around the theory, some of the arguments are tied to one version or another. For example, there was an experiment run a few years back that was billed as a "Experimental realization of a first test of de Broglie–Bohm theory". This based on Ghose's formulation, which has been denounced by other proponents of dBB. So some of the debate has my head spinning. :D
 
  • #40
DrChinese said:
The issue for me is that I am still learning about dBB/BM. Travis had never objected to me about the terminology, so what you say makes sense. He also talks about Bell's later writings a lot, so that makes sense too.


May I recommend then the most objective and diverse account of deBB theory in the literature:

What you always wanted to know about Bohmian mechanics but were afraid to ask
Authors: Oliver Passon
http://aps.arxiv.org/abs/quant-ph/0611032

Why isn't every physicist a Bohmian?
Authors: Oliver Passon
http://aps.arxiv.org/abs/quant-ph/0412119



DrChinese said:
As I look into the issues around the theory, some of the arguments are tied to one version or another. For example, there was an experiment run a few years back that was billed as a "Experimental realization of a first test of de Broglie–Bohm theory". This based on Ghose's formulation, which has been denounced by other proponents of dBB. So some of the debate has my head spinning. :D


Yes, Ghose's formulation is objected to for good reason. I recommend also this paper:

Comments on some recently proposed experiments that should distinguish Bohmian mechanics from quantum mechanics
Authors: W. Struyve, W. De Baere
http://arxiv.org/abs/quant-ph/0108038
 
  • #41
DrChinese said:
DGZ version ("Bohmian mechanics"): the guidance condition is fundamental and the quantum potential is de-emphasized. Bell preferred this version, as I understand it. Is Demystifier in this camp (not asking you to speak for him, just wonder if you happen to know)?
I'm in nobody's camp, but I prefer to think that the guidance law, and not the quantum potential, is the fundamental concept. I use the expression "Bohmian mechanics" not because it is the best name for it, but simply because most people use this term. Otherwise, I think that the expression "pilot-wave" is the best name, but I don't use it frequently for the reason explained above.
 
  • #42
Maaneli said:
May I recommend then the most objective and diverse account of deBB theory in the literature:

What you always wanted to know about Bohmian mechanics but were afraid to ask
Authors: Oliver Passon
http://aps.arxiv.org/abs/quant-ph/0611032

Why isn't every physicist a Bohmian?
Authors: Oliver Passon
http://aps.arxiv.org/abs/quant-ph/0412119

Yes, Ghose's formulation is objected to for good reason. I recommend also this paper:

Comments on some recently proposed experiments that should distinguish Bohmian mechanics from quantum mechanics
Authors: W. Struyve, W. De Baere
http://arxiv.org/abs/quant-ph/0108038

I read the second Passon paper (which was very good), and it definitely had my head spinning trying to follow the arguments and counter-arguments. Of course, there is no easy way out on it, so I'll have to continue to study.

Ditto for the Struyve-Baere comment, which Ghose answered: http://arxiv.org/abs/quant-ph/0208192

The difficulty is that each person has a point of view (as we all do), and it is not fully convincing for an author to try to counter arguments from the "other" side. The other side seems to remain unconvinced throughout much of the debate, and both sides end up declaring "victory". That makes it hard for me to see where there is a modicum of agreement between the sides. For example: after Ghose's paper and the Struyve-Baere comment (and the other) and Ghose's answer to the comment, the experiment was later performed. So I presume that those performing the experiment ultimately thought Ghose was right (else their time was wasted): http://arxiv.org/abs/quant-ph?papernum=0206196

This is one area in which the PhysicsForums threads is very beneficial, because the various positions can be better discussed in a back and forth manner. So my thanks to all of you for continuing to help me better understand the best that dBB/BM has to offer.
 
Last edited:
  • #43
Demystifier said:
I'm in nobody's camp, but I prefer to think that the guidance law, and not the quantum potential, is the fundamental concept. I use the expression "Bohmian mechanics" not because it is the best name for it, but simply because most people use this term. Otherwise, I think that the expression "pilot-wave" is the best name, but I don't use it frequently for the reason explained above.

Thanks! I am not trying to pigeon hole anyone, but it is definitely helpful to know a little about where folks stand.
 
  • #44
So what about this: can anyone point me to a reference that explains how entanglement works in dBB/BM?

I presume there must be something like the following:

f(Alice)=f(Bob) while Alice and Bob are entangled so that the "answer" to any observation of Alice and Bob will be suitably correlated. And I am imagining that f(Alice) is the Guidance equation or the Quantum potential, depending on your perspective. As I understand it, the correlation would not be due to a signal directly moving from Alice to Bob (or vice versa) instantaneously so much as the fact that conditions in the universe were applied identically on each. I see that Alice and Bob sprang from identical conditions (al least in PDC) but I understand that the rest of the universe exerts an impact on Alice and Bob as well.

I know I am wandering in the park on this, can anyone point me in the right direction?
 
  • #45
After doing a little searching, I am beginning to think my question is a bit more complex than I had realized. I found a couple of references:

EPR-Bell Nonlocality, Lorentz Invariance, and Bohmian Quantum Theory
Authors: K. Berndl (Munich), D. Duerr (Munich), S. Goldstein (Rutgers), N. Zanghi (Genova) (Submitted on 26 Oct 1995)[/url]

and

Bohmian trajectories for photons
Authors: P. Ghose (S.N.Bose Natl. Centr.), A. S. Majumdar (S.N.Bose Natl. Centr.), S. Guha (IIT Kanpur), J. Sau (IIT Kanpur) (Submitted on 14 Feb 2001[/url]

Now I see that reference 1 states: "Within this framework an EPR experiment can be described—the subsystems, while not explicitly interacting, are coupled by their common wave function (ta, tb)...Despite the presence of EPR-correlations, these do not permit the transmission of “signals”: From the results of measurements on system a alone, one can draw no inference about the possible interventions on system b—the kinds of experiments performed on system b..." which makes sense to me.

On the other hand, reference 2 says that some Bohmians question whether bosons have Bohmian trajectories as Fermions do: "Bohm and his coworkers have all along emphasized a fundamental difference between fermions and bosons in that fermions, in their view, are particles, whereas bosons are fields. This asymmetry in the Bohmian picture of fermions and bosons arose due to the absence, in their view, of a consistent relativistic quantum mechanics of bosons with a conserved four-vector current which is time-like and whose time component is positive."

They proceed to compute the Bohmian trajectories for a pair of PDC photons, developed from the Kemmer equation (like I have any idea what that is). One of the authors is Ghose, whose credibility is questioned by some on this board. He sometimes writes no-go type papers on various Bohmian hypotheses, but seems to be pretty familiar with the field.

So do either of these papers work as a starting point to understanding the constraints that must exist on a pair of entangled particles? It seems clear that for entangled Alice and Bob, their trajectories must evolve with a manner of symmetry.
 
Last edited by a moderator:
  • #46
DrChinese said:
After doing a little searching, I am beginning to think my question is a bit more complex than I had realized. I found a couple of references:

EPR-Bell Nonlocality, Lorentz Invariance, and Bohmian Quantum Theory
Authors: K. Berndl (Munich), D. Duerr (Munich), S. Goldstein (Rutgers), N. Zanghi (Genova) (Submitted on 26 Oct 1995)[/url]

and

Bohmian trajectories for photons
Authors: P. Ghose (S.N.Bose Natl. Centr.), A. S. Majumdar (S.N.Bose Natl. Centr.), S. Guha (IIT Kanpur), J. Sau (IIT Kanpur) (Submitted on 14 Feb 2001[/url]

Now I see that reference 1 states: "Within this framework an EPR experiment can be described—the subsystems, while not explicitly interacting, are coupled by their common wave function (ta, tb)...Despite the presence of EPR-correlations, these do not permit the transmission of “signals”: From the results of measurements on system a alone, one can draw no inference about the possible interventions on system b—the kinds of experiments performed on system b..." which makes sense to me.

On the other hand, reference 2 says that some Bohmians question whether bosons have Bohmian trajectories as Fermions do: "Bohm and his coworkers have all along emphasized a fundamental difference between fermions and bosons in that fermions, in their view, are particles, whereas bosons are fields. This asymmetry in the Bohmian picture of fermions and bosons arose due to the absence, in their view, of a consistent relativistic quantum mechanics of bosons with a conserved four-vector current which is time-like and whose time component is positive."

They proceed to compute the Bohmian trajectories for a pair of PDC photons, developed from the Kemmer equation (like I have any idea what that is). One of the authors is Ghose, whose credibility is questioned by some on this board. He sometimes writes no-go type papers on various Bohmian hypotheses, but seems to be pretty familiar with the field.

So do either of these papers work as a starting point to understanding the constraints that must exist on a pair of entangled particles? It seems clear that for entangled Alice and Bob, their trajectories must evolve with a manner of symmetry.



The first paper by Berndl et al. is a decent starting point, though they are more interested in pin-pointing the nature of the "conflict" between pilot-wave theory and Lorentz invariance. In terms of the critiques of reference 2, those issues about a positive, timelike 4-current for bosons are widely accepted to have been resolved in pilot-wave QFT generalizations of Struyve et al.:

A minimalist pilot-wave model for quantum electrodynamics
Authors: W. Struyve, H. Westman
Journal reference: Proc. R. Soc. A 463, 3115-3129 (2007)
http://arxiv.org/abs/0707.3487

Also have a look at:

On the uniqueness of paths for spin-0 and spin-1 quantum mechanics
Authors: W. Struyve, W. De Baere, J. De Neve, S. De Weirdt
Journal reference: Phys. Lett. A 322, 84-95 (2004)
http://arxiv.org/abs/quant-ph/0311098

If you would like to better understand how deBB theory accounts of EPRB correlations for electrons and other fermions, I recommend looking at Peter Holland's textbook, "The Quantum Theory of Motion", and Bohm and Hiley's "The Undivided Universe". They both have explicit discussions of EPRB for electrons from a pilot-wave point of view. Also have a look at page 74 of Genovese's review paper where he generally describes how deBB describes the Stern-Gerlach experiment:

Research on Hidden Variable Theories: a review of recent progresses
Authors: Marco Genovese
Journal reference: Physics Reports 413 (2005) 319
http://arxiv.org/PS_cache/quant-ph/pdf/0701/0701071v1.pdf
 
Last edited by a moderator:
  • #47
Maaneli said:
The first paper by Berndl et al. is a decent starting point, though they are more interested in pin-pointing the nature of the "conflict" between pilot-wave theory and Lorentz invariance. In terms of the critiques of reference 2, those issues about a positive, timelike 4-current for bosons are widely accepted to have been resolved in pilot-wave QFT generalizations of Struyve et al.:

A minimalist pilot-wave model for quantum electrodynamics
Authors: W. Struyve, H. Westman
Journal reference: Proc. R. Soc. A 463, 3115-3129 (2007)
http://arxiv.org/abs/0707.3487

Also have a look at:

On the uniqueness of paths for spin-0 and spin-1 quantum mechanics
Authors: W. Struyve, W. De Baere, J. De Neve, S. De Weirdt
Journal reference: Phys. Lett. A 322, 84-95 (2004)
http://arxiv.org/abs/quant-ph/0311098

If you would like to better understand how deBB theory accounts of EPRB correlations for electrons and other fermions, I recommend looking at Peter Holland's textbook, "The Quantum Theory of Motion", and Bohm and Hiley's "The Undivided Universe". They both have explicit discussions of EPRB for electrons from a pilot-wave point of view. Also have a look at page 74 of Genovese's review paper where he generally describes how deBB describes the Stern-Gerlach experiment:

Research on Hidden Variable Theories: a review of recent progresses
Authors: Marco Genovese
Journal reference: Physics Reports 413 (2005) 319
http://arxiv.org/PS_cache/quant-ph/pdf/0701/0701071v1.pdf

Thanks, I'll review these and come back with any questions.

-DrC
 
Back
Top